Digital differential analyzers



May 2, 1961 D. c. EVANS DIGITALDIFFERENTIALANALYzERs l Q A BY .NSQQC LMSC.

mh) WN Filed March l, 1954 D l 6 9 l 2., y m

Filed March l, 1954 NNN VEN

who@

www

May 2, 1961 D. c. EVANS DIGITAL DIFFERENTIAL ANALYzERs Filed March l, 1954 NNW NRM

MKM

Www-Mmmm WQQVSQQ NNM.

May 2, 1961 D. c. EVANS DIGITAL DIFFERENTIAL ANALYZERS 16 Sheets-Sheet 4 Filed March l, 1954 D. C. EVANS DIGITAL DIFFERENTIAL ANALYZERS May 2, v1961 16 Sheets-Sheet 5 Filed March 1, 1954 MNQEQM KSUNQU mkv@ www IN V EN TOR.

4 l//D C. EWINS www www

INN.

MKM

May 2, 1961 D. c. EVANS DIGITAL DIFFERENTIAL ANALYZERS 16 sheets-sheet e Filed March l, 1954 WSW IN VEN TOR.

DA l//D C, V4/V5 M KW ATTO/@WIV May 2, 1961 D. c. EVANS 2,982,470

DIGITAL DIFFERENTIAL ANALYZERS Filed March 1, 1954 1e sheets-sheet# I VEN TOR. .OAV/p C. EVA/vs Arrow/viv y bmw..

NIH

May 2, 1961 D. c. EVANS 2,982,470

DIGITAL DIFFERENTIAL ANALYZERS Filed March l, 1954 16 Sheets-Sheet 8 INVENToR. 0A l//D c, EMA/5 MKM@ May 2, 1961 D, c. EVANS DIGITAL DIFFERENTIAL ANALYZERS 16 Sheets-Sheet 9 Filed March 1, 1954 KS3@ m5@ Afro/wey 16 Sheets-Sheet 10 D C EVANS DIGITAL DIFFERENTIAL ANALYZERS May 2, 1961 Filed March 1, 1954 QM@ QW FSQQ`U KSUAXM mi@ E vm EL. -MM

MEQN

www

NSQQG mkv@ INVENTOR.

Al// C. EWMS ATTORNEY May 2, 1961 D. c. EvANs 2,982,470

DIGITAL DIFFERENTIAL ANALYzERs Filed March I, 1954 I6 sheets-sheet 11 IN VEN TOR. 94V/0 C M4/V5 8mm@ M Arma/5V May 2, 1961 D. C. EVANS DIGITAL DIFFERENTIAL ANALYZERS Filed March l, 1954 16 Sheets-Sheet 12 l @Je ELE-15 CHANNEL CHAN/VEL AAN/VEL INVENTOR.

May 2, 1961 Filled March l, 1954 D. C. EVANS DIGITAL DIFFERENTIAL ANALYZERS 16 Sheets-Sheet 15 mdff? dpa/12x,-

uffa/2X A21/(RMX) LJLE INVENTOR.

DAV/D C, lV/VS Afro/MEV May 2, 1961 D. c. EVANS 2,982,470

DIGITAL DIFFEREINTIALIY ANALYZERS Filed March l, 1954 16 Sheets-Sheet 14 INVENToR,

0A wa c. w1/v5 ...15 l BY E www Arro/VEV May 2, 1961 D. c. EVANS 2,982,470

DIGITAL DIFFERENTIAL ANALYZERS I Filed March 1, 1954 16 Sheets-Sheet 16 fuMfzm/-zfwseeff /o oo/o////z 30o/0//ooa/54 4'00////0,0/o55 5.0/00//00//56 aa/of//o/OOJ? aa//f//o//o39 g/ooo//of//4a ///o/0///oo/4z /4//o/////ao45 EJE IN V EN TOR.

DAV/ c. EVA/vs M a' m `Ur1ird5we Parent 0 DIGITAL DIFFERENTIAL ANALYZERS David C. Evans, Los Angeles, Calif., assigner to The University of Utah, Salt Lake City, Utah Filed Mar. 1, 1954, Ser. No. 413,058 j Claims. (Cl. 23561.6)I

This invention relates to digital differential analyzers and more particularly to apparatus lfor operating in conjunction with an analyzer to introduce empirical information to the analyzer for utilization by the analyzer. The invention also relates to apparatus for operating in conjunction with an analyzer to provide a permanent record of any particular quantity during and at the end of a computation.

4In U.S. Patent 2,900,134 issued to Floyd G. Steele and William S. Collison, a digital differential analyzer is disclosed for solving complex dilferential problems by digital steps. The analyzer has the advantages of both digital computers and differential analyzers. The analyzer obtains the advantages of differential analyzers in that it is relatively'simple in construction. The analyzer also has the advantage of digital computers in its speed and accuracy of operation. By combining these advantages, a computer is obtained which is able to solve complex dilierentialequations even though it is housed in a cabinet smaller than a desk.

Since the analyzer operates on a differential basis, it has a plurality of integrators which are interconnected in a particular manner in accordance with a mathematical problem which has to be solved. Because of these interconnections, quantities which are obtained by one integrator are introduced to other integrators to vary the quantities in these other integrators. Sometimes, however, it is necessary to introduce to an integrator empirical information which cannot be represented by a diiferential equation or in differential form.

This invention provides apparatus for operating in conjunction with a digital differential analyzer to introduce empirical information periodically and in digital form to manner in which the quantity varies during the solutionl of a problem.

An object of this invention is to'provide a digital differential analyzer which operates in digital steps to obtain a solution of complex differential problems.

Another object is to providel an analyzer of the above character which includes apparatus for introducing empirical nformatonrto the analyzer so as to increase the range of problems which can be solved by the analyzer. l A further object is to provide an analyzer of the above character which operates to receive empirical information periodically and in digital form from a permanent record such as a tape so yas to solve differential problems defined at least in part by such empirical information. j j Y Still another object is to provide apparatus for operating in conjunction with a'digtal ditferential analyzer to Ceg 2 provide a continuous record in permanent form of the value of a quantity computed by the analyzer.

A still further object is to provide a method of introducing empirical information Vto an analyzer for utiliza,- tion by the analyzer during the solution of a problem and of withdrawing computed information from the analyzer during the solution of the problem.

Other objects and advantages will be apparent from a detailed description ofthe invention and from the appended drawings and claims.

In the drawings: 4

Figure 1 is a simplied block diagram which schematically illustrates a digital differential analyzer forming one embodiment of this invention; j

Figures 2, 3, 4 and 5 are schematic diagrams, partly in block form aud partly in perspective, illustrating. in some detail certain of the electrical features constituting the digital'dilferential analyzer shown in Figure l;v`

Figures 6, 7 and 8 are schematic diagrams, partly in block form and partly in perspective, illustrating in some detail the cooperative relationship between certain of the electrical features and certain of the mechanical features constituting the invention; Y

Figures 9 and 10 areschematic diagrams, partly in block form and partly in perspective, illustrating in some detail other electrical features in the digital differential analyzer; Figure 11 is a circuit diagram of a bistable multivibrator which forms a basic stage of the analyzer' shown in Figure 1 andfin Figures 2 to l0, inclusive; Figure l2 is a block diagram illustrating the operatio of one .of the integrators forming part of the digital differential analyzer shown in Figure l and in Figures 2 to l0, inclusive; Y

Figure 13 is a curve illustrating the operation of an integrator such as the integrator shownin Figurel2;

Figure 14 is a chart which illustrates how dilerent parts of an integrator Vsuch as that shown in Figure 11 are coded to control the operation of the integratory.. Figure 15 is a schematic diagram illustrating the re.- lationship between dilferent integrators forming the-digital differential analyzer shown in Figure 1 and in Figures 2 to 10, inclusive, when the analyzer is solvingaparticularproblem; v ,A v Figure 16 is a chart illustrating the operationv of certain of components forming a part of the analyzer shown in Figure 1 and in Figures 2- to l0, inclusive; n

lFigure 17 is a chart illustrating the operation of cer tain of the components forming a part of the analyzer shown in Figure 1 and in Figures `2 to.10,inclusive,

v when the analyzer is undergoing a special form of com- (not shown). `A thin coating 12 (Figure 2) of magnetic material is applied to the ,periphery of the drum,` The coating 12 can be considered as being divided intoa plurality of annular channels 14, 16, 1s andzo. These channels are shown schematically n Figure 1v in separated relationship for purposes of convenience. AEach of the channels is separated by a sufficient distancewfrgiamV its adjacent channel so as to be substantially unaffected by the magnetic information provided in the adjacent channel. Y

.A 2,982,470 Patented May 2, 1,961

of a

The circumferential distance of each channel may be considered as being divided into a plurality of positions. Each of the positions is suiciently separated from its adjacent positions to receive a dilerent magnetization than that provided on the adjacent positions. For example, approximately 1,060 equally separated `pulse positionsmaybe provided in each channel when the drum has a radius of approximately 4inches. A

`A plurality of toroidal coils are positioned adjacent to each of the channels 14, 16, 18 and 20. For example, coils 22, 24 and 26 are provided in contiguous relationship to the channel 14. These channels are shown schematically in Figure 1. Similarly, coils 28;` 3 0 and 32 and coils 34, 36 and 38 are associated'luwith` thechannels 16 and 18, respectively. A' single coil 40 is disposed adjacentthe channel 20. y 4

The coils 22 and 26 are etfectively'separated from each other by approximately 104 pulse positions, and the coil 24 is` disposed at an intermediate positionv between the lcoils 22 and 26. The coil 26 is adapted to provide electrical signals in a pattern dependent upon the operation of the digital differential analyzer andto induce the corresponding magnetic pattern ony the drum 10 as the drum rotates. The pattern induced on the drum 10 by the coil 26 is of the binary form in which a magnetization in one circumferential direction indicates one value and a magnetization n the other direction indicates a second value.

The coil 22 is adapted to pick up the changes in the direction of magnetization in the channel 14 as the drum rotates and to produce corresponding electrical signals. The coil 28 is adapted to produce a substantially constant signal for returning the direction of magnetization on the drum to that representing a value of after the magnetic pattern on the'drum has been converted into a corresponding electrical pattern by the coil 22.

The coils 28, 30 and 32 in the channel 16 are separated from one another by distances Icorresponding to the distances between the coils 22, 24 and 26 and are adapted to perform functions similar to those performed by the coils 22, 24 and 26, respectively. The coils 36 and 38 in the channel 18 effectively separated from the coil 38 byy approximately 49 `pulse positions during the operation ofthe analyzer to obtain the solution of amathematical problem. The coil 36 is`disposed between the coils 34 and 38.

The coil 36 is adapted to operate in a manner similar 'to the coil-38 to convert electrical signals Vinto magnetic signals forl recordation in the channel 18.` The coil 38 -is adaptedto produce signals in accordance with the magnetic pattern provided in the channel 18 bythe coil 3 6. The coil 34 is adapted to operatein a manner similarto the coil124 to produce a 0 direction of 'magn'etization in the channel 18' after the pattern provided bythe coil 36 has been utilized by the coil 38.

The coil 40 is adapted toproduce an electrical signal approximating a sinewave as each pulse position in the channel 20 moves past the coil. The coil 40 produces sinusoidal electrical signals because of the magnetic pattern permanently provided in the channel 20. This pattern remains constant regardless of the problem to be solved.

A counter 42 is connected to the coil 40 to count the sinusoidal electrical signals in the channel 20 as the drum rotates. VThe counter 42 may be formed from a plurality of bistable multivibrators connected in cascade arrangement and is adapted to count successive sine signals in a numerical range from 1 to 48. Upon each count of 548,. the counter 42Yis adapted to return to its initial statefor the commencement of a new count. As will bedisclosed hereinafter, anew integrator is presented for computation upon the completion of each count of 48.

Similarly, a counter 44 may be formed from a plurality of b isitablewmultivibrators in cascade arrangement. The counter 44 is connected to the counter 42 to count the number of times that a full count is obtained in the counter 42. For example, the counter 44 may count up to 22 full counts in the counter 42 before returning to its initial state for the initiation of a new count. ln this way, the counters 42 and 44 divide the drum 10 into 22 integrator sections, each having 48 pulse positions. The construction and operation of the counters 42 and 44 are fully disclosed in U.S. Patent 2,900,134 issued to Floyd G. Steele and William S. Collison. As schematically shown in Figure 1, the output signals induced in the coil 22 are introduced to` a gate circuit 46 which also has signals applied to it through a line 48 from the counter 42. The output signals from the gate circuit 46 are in turn applied through an or4 network 50 to the coil 26 for recordation in the channel 14. The systems described herein include two types of logic circuits, and gates and or networks. In the figures, the or networks are shown as triangles while the and gates are represented by rectangles. Both of these circuits are used in conjunction with two-state signals; An and gate provides a high two-state signal at its output when all its input signals are at a high state, while an or network provides a high output when any of its inputs are high. To avoid confusion herein, and gates will be referred to hereinafter as simply gates and or networks will be referred to as or networks. Similarly, a gate circuit 52 receives signals from the coil 28 and through the line 48 from the counter 42. The output terminal of the gate circuit 52 is connected to an input terminal of an or network 54 having its output terminal connected to the coil 32.

The output signals from the gate circuit 46 are not only applied to the or network 50 but also to gate circuits 56 and 58. The gate circuit 56 also receives signals from the coil 38, and the gate circuit 58 has signals introduced to it from an inverter 60 connected to the coil 38. The output signals from the gate circuits 56 and 58 respectively pass to the grids of the left and right tubes in a bistable multivibrator`60.

Similarly, connections are made to input terminals of a gate circuit 62 from the gate circuit 52 and from the coil 38 and to input terminals of a gate circuit 64 from the gate circuit 52 and the inverter 60. The output terminals of the gate circuits 62 and 64 are connected to a counter 66, which may be formedffrom a plurality of multivibrators (not shown) in cascade arrangement. The construction and operation" of the counter 66 are fully disclosed in U.S. Patent 2,900,134.

The output signals from the counter 66 pass to input terminals of a gate circuit 68, another input terminal of which is connected to the plate of the left tube in a bistable multivibrator 70. The grid of the left tube in the multivibrator 70 receives its voltage from the output terminal of a gate circuit 72 having input terminals connected to the coil 28 and through a line,74 to the counter 42. The grid of the right tube in the multivibrator 70 is connected through a line 76 to the counter 42.

The signals passing through the gate circuit 68 are introduced to input terminals of an adder 78. Another input terminal of the adder 78 receives the signals from a carry circuit 80, the input'terminal of which is connected to the output terminal of theadder 78. Signals are also introduced to the adder 78 from a gate circuit 82 having input terminals connected to the coil 7.3 and to the plate of the left tube in the multivibrator 70. The operation of the adder 78 is controlled by the voltage on the plate of the left tube in a multivibrator 84. The operation of an adder 86 Vis also controlled by the voltage on the plate ofthe left tube in the multivibrator 84. The adder 86 receives for arithmetical combination the signals from the gate circuits 72 and82. The adder 86 also receives for arithmetical combination the signals from a carry circuit 90, the input terminal of which is connected to the outputterminal of the adder. Conner. tionsfare made from the plates of the left and `righttubes in the multivibrator 60 to` the adder 86to controltbe particular manner in which the different signals are arith` metically combined by the adder., The output from the adder is introduced through the or network 50 to the coil 26 for recordation in the channel 14.

The output from the adder 86 passes to a gate circuit 92 having other input terminals connected to the plate of the leftl tube in the multivibrator 84 and through a line 76 to the counter 42. The signals 'passing through the gate circuit 92 are applied through an or network 94 to the coil 36 for recordation in the channel 18. Signals are also applied to the or network 94 from a gate circuit 96, input terminals of 'which are connected to the coil 38, to the plate of the left tube in the multivibrator 84 and through a line 97 to the counter 42.

In addition to being connected to the gate circuit 92, the output terminal of the adder 86 is connected to an input terminal of a gate circuit 98 having other input terminals connected through the line 76 to the counter 42 and through a line 100 to the counter 44. The signals passing through the gate circuit 98 are introduced to the grid of the right tube in the multivibrator 84. The plate of the right tube in the multivibrator' 84 is con nected to input terminals of gate circuits 104, 106 and 108 to control the operation of these circuits.

'Ihe gate circuit 104 has other input terminals connected to the coil 22 and to an inverter 110 the operation of which is controlled by signals passing through a line 112 from the counter 44. The output signals from the gate circuit 104 are applied through lthe or network 50 to the coil 26 for recordation in the channel 14. Similarly, connections are made to other input terminals of the gate circuit 106 from the coil 28 and the inverter 110 and the output from the gate circuit 106 is introduced to the or network 54 'for recordation by the coil 32 in the channel 16. The gate circuit 108 has an input terminal connected to the coil 38 as well as to the plate of the right tube in the multivibrator 84. The signals passing through the gate circuit 108 are introduced to the or network 94 for recordation by the coil 36 in the channel 18.

The voltage on the plate of the right tube in the multivibrator 84 is also introduced to a gate circuit 116 having other input terminals connected through the line 76 to the counter 42 and through the line 100 to the counter 44. The output from the gate circuit 116 is introduced to thegrid of a normally conductive left tube in a monostable multivibrator 118 to trigger the tube into nonconductivity. The plate of the left tube in the multivibrator 118 is connected to a counter 120 which may be formed from a plurality of multivibrators connected in a cascade arrangement to provide only a positive and sequential count. A connection is also made from the plate of the left tube in the multivibrator 118 to a tape reader 122 and a tape puncher 124. The construction and operation of the tape reader 122 and the tape puncher 124 will be disclosed in detail hereafter.

Connections are made from the output terminal of the counter 120 to the grid of the left tube in the multivibrators 84 and to input terminals of gate circuits 126 and 128. The gate circuit 126 has other input terminals connected to the tape reader 122, through a line 130 to the counter 42 and through the line 112 to the counter 44. The output signals from the gate circuit-126 are introduced through the or network 54 to the coil 32 for recordation in the channel 16. In addition to being connected to the counter 120, input terminals of the gate circuit 128 are connected to the coil 28, through the line 130 to the counter 42 and through a line 132 to the counter 44. The output signals from the gate circuit 128 operate the tape puncher 124 to provide a permanent record of the information represented by the signals.

The digital dierential analyzer disclosed above in simpliiied form is adapted to provide the solution of differental equations. For example, it may providerthe Y t@ solution of the problem of fydx=ff(x)dx, where f(x) represents a function of x and ff(x)dx represents the integral of the function. If a curve y=f(x) is plotted with x as the abscissa andy as the ordinate, the analyzer obtains the relationship fydx=ff(x)dx by computing the area under the curve y=f(x). By determinining the area under the curve y=;f(x), the analyzer performs electronically operations which may sometimes be performed mentally by a skilled mathematician when the problem to be solved is relatively simple.

The analyzer obtains the value of the function fydx=ff(x)dx by producing small increments of x. These increments may be represented by the symbol Ax. For each Ax increment, the analyzer determines the value of y and obtains the product yAx. This product yAx approximates the areaunder the curve y=f(x) for each Ax increment, as indicated in Figure 13 by the shaded area for a particular Ax increment. If the product yAx is obtained for successive Ax increments and if all of the yAx increments are added together, the area under the interval of the curve representing f(x) from x0 to x may be approximated. A relatively accurate approximation may be obtained by decreasing the value of each Ax increment.

An integrator for determining the yAx increments and for storing the cumulative values of these increments is shown in Figure l2. The integrator includes a transfer stage 142 for obtaining Ax increments at periodic intervals through a line 144. The integrator also has an integrand accumulator 146 for storing the value of the dependent quantity y and for receiving Ay increments through a line 148 from its own and from other integrators so as to vary the value of y in accordance with the function y=f(x).` An output accumulatork 150 is provided to receive yAx increments, to combine each yAx increment with the previous increments and todeliver the'cumulative value obtained to another integral accumulator or transfer stage while holding the remainder in store. hereafter.

The interrelationship between diierent integrators is illustrated in Figure 15 for a particular problem. This problem starts with a differential equation represented by A detailed explanation of this willbe given to obtain the function y=tan x are indicated in Figure y l 15 by blocks 152, 154 and 156. The generation of the function x tan x from the function tan x is accomplished by blocks 158 and 160 shown in Figure 15. The value 5 of the function x tan x at any instant is accumulated in l the integrator 160. In each of the integrators in Figure 15, the introduction of the Ax increments constituting Y changes in the independent variable quantity for the integrator is indicated by a line extending into the upper right position in the block. The Ay increments are introduced into the integrator through a line or a plurality of lines extending into the lower right portion of 'the block representing the integrator. The output ofthe integrator is obtained from a line extending from anY interv mediate position at the right side of the appropriate block.

, As will be seen in Figure l5, Ax increments of ythe independent variable quantity fora particular integrator may be obtained from the Voutput of another'integrator.

evaluating the integral of-a i general equation y=f(x) so as to obtain a function For example, in Figure 15, the Ax increments for the integrators 154 and 156 are obtained from the output of the integrator 152. Similarly, Ay increments for a particular integrator may be obtained from the output of other integrators as well as from the output of the integrator itself. For example, Ay increments for the integrators 154 and 158 are obtained from the output of the integrator 152.

The Ax and Ay increments-for each integrator are actually determined from a coded pattern provided in the channels 14 and 16, respectively. As previously disclosed, the pulse positions in each channel are subdivided into 22 integrators each having 48 pulse positions. The tirst 22 positions in each integrator in the channel 14 are coded to indicate a Ax increment. Since the first 22 positions in the channel 14 for each integrator section correspond in number to the 22 integrators in the analyzer, each integrator can receive a Ax increment from the output of any of the other integrators. This can be eiectuated by providing a pulse in the channel 14 in a particular one of the first 22 positions for the integrator.

For example, the Ax increments for the integrator 154 in Figure 15 would be coded in a particular one of the 22 positions in the channel 14. As will be disclosed in detail hereinafter, the particular position corresponds to the time at which the output from the integrator 152 appears on the coil 38. In Figure 14, a pulse 162 is shown as being recorded in the channel 14 in the 11th pulse position of a particular integrator section.

A pulse in the channel 14 in one of the rst 22 positions for a particular integrator indicates that a Ax increment is to occur for the integrator. However, such a pulse does not indicate the polarity of the Ax increment. The polarity of the Ax increment for the integrator iS indicated by the presence or absence of a coincidental pulse in the channel 18. If a positive pulse is picked up from the channel 18 by the coil 38 at the same time as the pulse representing the Ax increment for a particular integrator is picked up by the coil 22, the Ax increment for the integrator is positive. For example, the pulse 162 in Figure 14 indicates a positive Ax increment for a particular integrator since it coincides in time with a pulse 164 in the channel 18. A negative Ax increment occurs for an integrator if a positive pulse does not appear in the channel 18 at the same time as the pulse in the channel 14.

The iirst 22 positions in the channel 16 for each integrator are coded to indicate Ay increments in a manner similar to the coding of corresponding positions in the channel 14 to indicate Ax increments. Since the first 22 positions in each integrator section correspond to the 22 integrators in the digital differential analyzer, each integrator section is coded with particular ones of the first 22 positions in the channel 16 so as to receive the output from certain other integrators in accordance with the problem to be solved. For example, a pulse is coded in the channel 16 in a particular one of the iirst 22 positions for the integrator 15S in Figure 15 so as to coincide with the time at which the output from the integrator 152 is made available to the coil 3S in the channel 18. Although only one Ax increment can be obtained for an integrator upon each presentation of the integrator for computation, several Ay increments can be obtained. This may be Seen by the pulses 168 and 170 in the channel 16 in the Figure 14.

Each pulse in the rst 22 positions in the channel 16 for each integrator represents a Ay increment, but it does not indicate the polarity of such an increment. The polarity of the increment is indicated by the presence or absence of a pulse in the channel 18 at the time that a coding pulse is` induced in theeoil 28. For example, the pulse 168 in Figure 14 indicates a positive Ay increment for a particular integratorsince it coincides in time with a pulse 172 in the channel 18. However, a negative Ay increment is obtained when the pulse is picked up by the coil 28 since there is no coincidental pulse in the channel 18.

Since the interrelationship between the different inte` grators remains constant during the solution of a partielllar problem, the coding pulses in the channels 14 and 16 for the first 22 positions from each integrator section must be retained during the computation. Retention of the pulses in the channel 14 is etectuated by the gate circuit 46, which remains open during the first 22 positions for each integrator to pass the coded information in these positions. This is indicated in Figure l by the indication P1-P22 adjacent the line 48 from the counter 42 to the gate 52, indicating that the line 48 carries a high signal during the first twenty-two pulse positions of each integrator storage section. The gate circuit 46 opens during these positions because of the introduction of a relatively high voltage through the line 48 from the counter 42. The signals then pass through the or network 50 for recordation by the coil 26 in the channel 14. Similarly, the gate circuit 52 opens during the first 22 positions for each integrator so that the coding infomation in the channel 16 can pass through the or network 54 for recordation by the coil 32 in the channel.

It should be appreciated that the gate circuits similar to the circuit 46 operate to pass information only when positive pulses are simultaneously introduced to all of the input terminals of the circuit. In computer terminology, sueh circuits have been designated as and networks. The term or networks is also common in computer terminology. Such circuits operate to pass information when any one of their input terminals receives a relatively high voltage. Such or networks are shown in the drawing as triangles and are exemplified by the networks 50 and 54.

During the tirst 22 positions of each integrator, the gate circuits 62 and 64 operate to determine the polarity of each Ay increment for the integrator. The gate circuit 62 determines the positive Ay increments by passing a signal only when a positive signal is produced by the coil 38 at the same time that a signal passes through the gate circuit 52 to indicate a coding pulse in the channel 16. Because ot' the inversion by the inverter 60 of the pulses induced in the coil 38, the gate circuit 64 passes a signal only when a relatively low voltage is induced in the coil 38 to indicate a negative value. Since the gate circuit 64 passes a signal only when the inverted voltage coincides with a coding pulse in the channel 16, the gate circuit passes signals to indicate negative Ay increments.

At the same time that the gate circuits 62 and 64 operate to determine the polarity of each Ay increment for an integrator, the counter 66 arithmetically combines such increments. For example, a signal passing to the counter 66 from the gate circuit 62 may cause the circuit to provide a numerical indication of +4 when an indication of +3 was previously provided by the counter. Similarly, the indications in the counter 66 may change from a value of -2 to a value of -3 upon the introduction of a signal from the gate circuit 64.

The counter 66 retains in binary form the numerical information relating to the cumulative value of the Ay increments for an integrator. The counter 66 retains the information in binary form since it comprises a plurality of multivibrators arranged in cascade relationship. In a more complex embodiment, four multivibrators in eascade arrangement are provided. 'For example, with a resultant count of +5 for the Ay increments for a particular integrator, the first and third multivibrators in the cascade arrangement may be operated to indicate a binary' pattern of 0101, where the least significant digit is at the right. In binary form, a pattern of 0101 indicates that (0)(23)l(1)(22)l(0)(21)|(1)(2)=5 Similarly, a value of +3 is indicated by a pattern of 0011, where the least significant digit is at the right. In this embodiment, a single multivibrator is illustratively used to count the 

